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NUMERICAL SIMULATION OF RAYLEIGH-TAYLOR INSTABILITY IN ABLATION DRIVEN SYSTEMS.VERDON, CHARLES PETER. January 1984 (has links)
Two-dimensional numerical simulations of ablatively accelerated thin-shells subject to Rayleigh-Taylor instability are presented. Results for both single wavelength and multiwavelength perturbations show that the nonlinear effects of the instability are evident mainly in the "bubble" rather than the "spike." Approximate roles for predicting the dominant nonlinear mode-mode interactions, which limit shell performance, are also discussed. The work concludes with a discussion of recommendations for future work in this area.
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Modeling transient thermalhydraulic behavior of a thermionic fuel element for nuclear space reactorsAl-Kheliewi, Abdullah S. 20 September 1993 (has links)
A transient code (TFETC) for calculating the temperature
distribution throughout the radial and axial positions of a
thermionic fuel element (TFE) has been successfully developed.
It accommodates the variations of temperatures, thermal power,
electrical power, voltage, and current density throughout the
TFE as a function of time as well as the variations of heat
fluxes arising from radiation, conduction, electron cooling,
and collector heating. The thermionic fuel element transient
code (TFETC) is designed to calculate all the above variables
for three different cases namely: 1) Start-up; 2) Loss of flow
accident; and 3) Shut down.
The results show that this design is suitable for space
applications and does not show any deficiency in the
performance. It enhances the safety factor in the case of a
loss of flow accident (LOFA). In LOFA, it has been found that
if the mass flow rate decreases exponentially by a -0.033t,
where t is a reactor transient time in seconds, the fuel
temperature does not exceed the melting point right after the
complete pump failures but rather allows some time, about 34
seconds, before taking an action. If the reactor is not shut
down within 34 seconds, the fuel temperature may keep
increasing until the melting point of the fuel is attained. On
the other hand, the coolant temperature attains its boiling
point, 1057 ��K, in the case of a complete pump failure and may
exceed it unless a proper action to trip the reactor is taken.
For 1/2, 1/3, and 1/4 pump failures, the coolant temperatures
are below the boiling point of the coolant. / Graduation date: 1994
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Model of an ablating solid hydrogen pellet in a plasmaParks, Paul B. January 1979 (has links)
Thesis--University of Illinois at Urbana-Champaign, 1977. / Includes bibliographical references (p. 126-128).
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STATIONARY FLOW MODEL OF ABLATIVELY IMPLODED INERTIAL CONFINEMENT FUSION TARGETS.MONTIERTH, LELAND MELVIN. January 1982 (has links)
The steady flow model is applied to ablatively accelerated spherical targets for inertial confinement fusion. A parameter study is conducted which identifies regions of good hydrodynamic efficiency. In the limit of very large acceleration the model is seen to become planar and can be used to treat some large aspect ratio shells. A model of charged particle beam driven ablation is presented. The ablation resulting from this form of energy deposition can resemble laser driven albation in some cases, but qualitatively different behavior occurs in certain regimes of the beam power and range. Laser energy deposition by inverse bremsstrahlung is also included. A procedure for descaling the dimensionless results of the steady flow model is presented. This allows for comparison of the model with experiments and numerical simulations.
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